Magnetar field dynamics driven by chiral anomalies without magnetic helicity
无磁螺旋度下手征反常驱动的磁星磁场动力学
The chiral magnetic effect (CME), arising from the chiral anomaly and enabling a mutual conversion between magnetic topology and fermionic chirality, is a key mechanism in magnetar field evolution. In previous work, Dehman and Pons [Phys. Rev. Res. 7, 033231 (2025).PPRHAI2643-156410.1103/rhv5-nd4v] demonstrated that the CME can efficiently generate dipolar fields (<inline-formula><mml:math><mml:msub><mml:mi>B</mml:mi><mml:mrow><mml:mi>dip</mml:mi></mml:mrow></mml:msub><mml:mo>≳</mml:mo><mml:msup><mml:mn>10</mml:mn><mml:mn>14</mml:mn></mml:msup><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>G</mml:mi></mml:math></inline-formula>), consistent with magnetar timing measurements, provided that the initial magnetic field carries net helicity. However, whether neutron stars are born with magnetic helicity remains uncertain. In this work, we investigate the CME across a range of initial helicity configurations, including nonhelical initial conditions. We find that the CME efficiently generates magnetar-strength dipoles on timescales of decades, independently of the initial helicity content. The chiral instability is driven by localized helical structures that induce a residual chiral asymmetry and is primarily governed by the maximum chiral chemical potential, requiring <inline-formula><mml:math><mml:msubsup><mml:mi>μ</mml:mi><mml:mn>5</mml:mn><mml:mi>max</mml:mi></mml:msubsup><mml:mo>≳</mml:mo><mml:mi>few</mml:mi><mml:mo>×</mml:mo><mml:msup><mml:mn>10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn>11</mml:mn></mml:mrow></mml:msup><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>MeV</mml:mi></mml:math></inline-formula> for onset in the magnetar regime. Our results further show that these dipoles may either remain stable and subsequently evolve through standard Ohmic decay, or become unstable if they acquire sufficient helicity, in which case they decay through the chiral anomaly, transferring energy to less helical modes. This outcome depends sensitively on the initial helicity distribution. These findings extend the applicability of the CME to more realistic magnetic-field configurations and underscore the importance of the helicity distribution at birth; a quantity that remains poorly constrained in newborn neutron stars, yet is crucial for determining their magnetic evolution and the emergence of magnetars.
展开 ▾证明 CME 在初始净磁螺旋度为零时仍能在数十年内生成约 10^14 G 的磁星偶极场;触发与效率由局部 μ5max 而非全局磁螺旋度控制,初始螺旋度分布决定所生成偶极场是否稳定。
前作 Dehman & Pons 2025 已证明,若初始磁场携带净螺旋度,手征磁效应可通过反级联形成磁星级偶极场;但新生中子星是否具有净磁螺旋度仍不确定。原初中子星磁场的 MHD 模拟通常得到以小尺度、非轴对称为主而大尺度偶极较弱的构型(Reboul-Salze+ 2021),这使无净螺旋度下 CME 是否可用成为关键问题。本文通过 MATINS 改变初始螺旋度含量与空间分布,发现局部螺旋结构即可支撑最大手征化学势并触发不稳定,在数十年内建立约 10^14 G 的偶极场,从而把 CME 推广到更接近真实诞生的磁场形态。展望上,下一步应耦合当前被忽略的霍尔项与 CME;已有结果表明霍尔反级联在中子星地壳中受纵横比限制(Dehman & Brandenburg 2025),而完整的 CME–Hall 耦合将有助于约束诞生时的磁螺旋度分布,并解释磁星、低场磁星与中央致密天体等观测类别的分化。
预印本 2026-05-08 · 刊出 2026-08-03 · 收录 2026-08-20